2014
DOI: 10.1016/j.compgeo.2013.09.004
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Particle simulation of thermally-induced rock damage with consideration of temperature-dependent elastic modulus and strength

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Cited by 54 publications
(11 citation statements)
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“…The temperature evolution of the granite specimen and the thermal cracking process are shown in Figure 25. With an increase in temperature, cracks initiate from the outer boundary of the specimen, gradually extend to the inside of the specimen along the radial direction, and finally extend to the hole at the center of the sample, as shown in Figure 25 from t = 4296 s to t = 11 814 s. The thermal cracking morphology obtained by the numerical model is similar to the fracture morphology observed in the laboratory 52 and previous numerical simulation results, 13 as shown in Figure 26. In addition, it can be clearly seen from t = 9129 s to t = 11 814 s in Figure 24 that there is a significant discontinuity in the temperature distribution at the cracks, which indicates that the 3D thermo-mechanical coupling model can account for the hindering effect of the crack dynamic extension on the heat transfer.…”
Section: Thermal Cracking Experimentssupporting
confidence: 81%
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“…The temperature evolution of the granite specimen and the thermal cracking process are shown in Figure 25. With an increase in temperature, cracks initiate from the outer boundary of the specimen, gradually extend to the inside of the specimen along the radial direction, and finally extend to the hole at the center of the sample, as shown in Figure 25 from t = 4296 s to t = 11 814 s. The thermal cracking morphology obtained by the numerical model is similar to the fracture morphology observed in the laboratory 52 and previous numerical simulation results, 13 as shown in Figure 26. In addition, it can be clearly seen from t = 9129 s to t = 11 814 s in Figure 24 that there is a significant discontinuity in the temperature distribution at the cracks, which indicates that the 3D thermo-mechanical coupling model can account for the hindering effect of the crack dynamic extension on the heat transfer.…”
Section: Thermal Cracking Experimentssupporting
confidence: 81%
“…Comparison of the final crack morphology of cylindrical specimens: A, results obtained by the 3D thermo‐mechanical coupling model; B, experimental results; C and D, results obtained by particle flow code [Colour figure can be viewed at wileyonlinelibrary.com]…”
Section: Thermal Cracking Experimentsmentioning
confidence: 99%
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“…To resolve heat conduction in the particle system, Feng et al [7] presented a 2D model where contacting circular particles share heat flux bonds with their neighbours; such models also exist in 3D using spherical particles [22]. When combining the thermal and bonded particle type of models, thermal fracturing was achieved by Xia et al [32,33] for circular particles and by Andre et al [2] for spherical particles. Among particle-based methods, we also find the peridynamic method [27] which was the principal advantage that its governing equations stay valid over discontinuities.…”
Section: Introductionmentioning
confidence: 99%
“…Meng et al [10] established a rock damage model considering freeze-thaw effect and discussed the total damage variables under freeze-thaw load from the aspects of damage area and microelement damage. Xia et al [11,12] believed that under the action of temperature, the linear expansion coefficient of each component in the rock is different, which leads to the thermal stress between particles. When the thermal stress exceeds a certain strength, new defects will be generated, and the thermal damage in the rock will be generated and developed.…”
Section: Introductionmentioning
confidence: 99%